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Electronic Structures and Spectral Properties of Endohedral Fullerenes Coordination Chemistry Reviews 249 (2005) 1111–1132 Review Electronic structures and spectral properties of endohedral fullerenes Suchi Guhaa,∗, Kazuo Nakamotob a Department of Physics and Astronomy, University of Missouri, Columbia, MO 65211, USA b Department of Chemistry, Marquette University, P.O. Box 1881, Milwaukee, WI 53217, USA Received 29 September 2004; accepted 8 November 2004 Available online 5 January 2005 Contents 1. Introduction ........................................................................................................ 1112 2. Theoretical background.............................................................................................. 1112 2.1. A simple model for the electronic structure of C60 ................................................................ 1112 2.2. Quantum chemical methods.................................................................................... 1113 2.3. Ab initio calculations of endohedral fullerenes ................................................................... 1114 2.4. Vibrational spectra ............................................................................................ 1115 2.4.1. Raman intensity calculations ........................................................................... 1115 2.4.2. IR absorption intensity calculations ..................................................................... 1116 3. C60 and C70 ........................................................................................................ 1116 3.1. Electronic states of alkali-doped exohedral C60 ................................................................... 1117 3.2. Endohedral C60 and C70 ....................................................................................... 1118 3.2.1. Kr@C60 ............................................................................................. 1118 3.2.2. Li@C60 .............................................................................................. 1119 3.2.3. M@C60 (M: rare-earth metal) .......................................................................... 1120 4. C72 and C74 ........................................................................................................ 1121 4.1. Ca@C72 and Ca@C74 ......................................................................................... 1121 4.2. Eu@C74 ..................................................................................................... 1122 5. C78 ................................................................................................................ 1122 6. C80 ................................................................................................................ 1123 6.1. La2@C80 .................................................................................................... 1123 6.2. Sc3N@C80 ................................................................................................... 1124 7. C82 ................................................................................................................ 1126 8. C84 ................................................................................................................ 1128 9. Summary and prospect .............................................................................................. 1130 Acknowledgements...................................................................................................... 1130 References.............................................................................................................. 1130 Abstract Endohedral fullerenes belong to a new class of compounds which are technologically and scientifically important owing to their unique structures and optoelectronic properties. This review focuses on theoretical calculations and spectroscopic (electronic, vibrational, and nuclear magnetic resonance (NMR)) studies of endohedral fullerenes thus far published. A theoretical background, with various computational ∗ Corresponding author. Tel.: +1 573 8843687; fax: +1 573 8824195. E-mail address: [email protected] (S. Guha). 0010-8545/$ – see front matter © 2004 Elsevier B.V. All rights reserved. doi:10.1016/j.ccr.2004.11.017 1112 S. Guha, K. Nakamoto / Coordination Chemistry Reviews 249 (2005) 1111–1132 methods used for determining energy-optimized electronic structure and calculation of vibrational spectra, is presented. Further, theoretical and spectroscopic investigations of individual endohedral fullerenes are discussed. Such studies provide structural information about the carbon cage, position of the encapsulated species, and the degree of charge transfer. In particular, 13C NMR spectroscopy is indispensable for the determination of the cage symmetry. In some cases, NMR signals from 45Sc encapsulated species yield information about dynamic behavior inside the cage. Vis–NIR absorption spectra determine the HOMO–LUMO band-gap energy. IR and Raman spectroscopy play an important role in elucidating the nature of interaction between the cage and encapsulated species. Novel vibrations resulting from these interactions appear in the low-frequency region, and the corresponding force constants serve as a measure of the strength of their interaction. © 2004 Elsevier B.V. All rights reserved. Keywords: Endohedral fullerenes; Density functional theory; UV–vis–NIR spectra; IR spectra; Raman spectra; C60;C70;C72;C74;C78;C80;C82;C84 1. Introduction have revealed the structure of the fullerene cages, the elec- tronic states of metal atoms and fullerene cages, and how It was first proposed in 1985 that fullerenes could confine the electronic properties and chemical reactivities of empty atoms in their interior because of their closed-cage structure fullerene cages change upon endohedral metal doping. Re- [1]. Since then metal-containing endohedral fullerenes have cently, these investigations have been extended to endohe- attracted special attention as a new class of technologically dral fullerenes containing small molecules, such as Sc3N and relevant materials due to their combined fullerene-like and Y2C2. In this section we give a brief overview of some of the metallic properties. In most endohedral metallofullerenes, theoretical techniques of modern quantum chemistry that are introduction of metal atoms into carbon cages leads to an used for the electronic and vibrational structure calculations increase in the electron affinity relative to the corresponding of fullerenes and endohedral fullerenes. empty-cages [2,3]. Endohedral metallofullerenes hold great promise for applications in optoelectronic devices since vary- 2.1. A simple model for the electronic structure of C60 ing the encapsulated metal cluster can alter the optical and electronic properties, without changing the structural features For a perfectly spherical molecule, one can use spherical of the outer carbon shell. Enhancement of third-order non- harmonics to predict the electronic energy levels. A model linear optical susceptibility observed in endohedral metallo- for the electronic structure of C60 based on elementary quan- fullerenes further establishes them as potential candidates for tum mechanics and group theory can be found in Ref. [10]. nonlinear optical devices [4]. The spherical nature of a C60 molecule allows the electronic A variety of endohedral metallofullerenes have been re- states to be labeled by spherical harmonics [11]. In this sim- ported, but their investigations have been severely limited plest model the 60 ␲ electrons of C60 are described by spher- because they are typically formed in extremely low yields ical harmonic wavefunctions modified slightly by the icosa- (<0.5%). This article is intended to review the structural and hedral symmetry. To accommodate 60 electrons according spectroscopic investigations of the limited number of endohe- to the Pauli exclusion principle and Hund’s rule, the energy dral fullerenes thus far published [5–7] and for which UV–vis states corresponding to =0 to = 4 are completely filled. and vibrational data are available. These studies have shed The highest energy level corresponding to = 5 has 10 un- light on the effect of encapsulation on the carbon cage, the paired electrons. Since pristine C60 is an insulator and has no location of the encapsulated species inside the cage, and the unpaired electrons, the above scheme needs to be modified. nature of interaction between the carbon cage and the encap- One has to invoke the icosahedral symmetry which is a lower sulated species. This review is organized as follows: Section symmetry compared to a perfect sphere. The carbon-derived 2 gives a theoretical background on electronic structure cal- potential splits the degenerate energy levels above = 2 of the culation of fullerenes and empirical models for Raman and spherical potential. The = 5 shell with 11 degenerate states infrared absorption intensity calculations. In Sections 3–8 we splits into a five-fold degenerate highest occupied molecular discuss the following fullerene cages: C60 and C70,C72 and orbital (HOMO), a threefold degenerate lowest unoccupied C74,C78,C80,C82, and C84. In each of these sections, we molecular orbital (LUMO) and an additional threefold de- first discuss the structure of empty fullerene cages followed generate level at a higher energy, as shown in Fig. 1. Fifty ␲ by a discussion of their endohedral counterpart in terms of electrons fill orbitals from = 0 to 4 and 10 electrons occupy the electronic states, electronic and vibrational spectra, and part of the
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